TABLE I.

Distances between fluorine and hydrogen atoms and F–H–F angles within the bifluoride anion in the gas phase, as well as Pnma HF at 300 GPa, and their corresponding crystal orbital Hamilton populations integrated to the Fermi level (-iCOHP). These same quantities are given for the bifluoride ions present within the Li–F–H phases at 300 GPa.

Bond−iCOHP
Distance (Å)angles (°) (eV/bond)
SystemF1–HF2–HF–H–FF1–HF2–H
(F–H–F) 1.160 1.160 180.0 3.61 3.61 
HF 1.047 1.048 175.3 7.46 7.09 
LiF2Ha 1.037 1.037 180.0 6.89 6.89 
LiF2Ha 1.034 1.067 165.3 7.10 6.33 
Li3F41.041 1.041 180.0 6.95 6.95 
LiF4H4 1.035 1.042 175.5 7.33 7.06 
Li2F31.041 1.041 180.0 6.96 6.96 
LiF31.014 1.079 180.0 7.81 6.22 
Bond−iCOHP
Distance (Å)angles (°) (eV/bond)
SystemF1–HF2–HF–H–FF1–HF2–H
(F–H–F) 1.160 1.160 180.0 3.61 3.61 
HF 1.047 1.048 175.3 7.46 7.09 
LiF2Ha 1.037 1.037 180.0 6.89 6.89 
LiF2Ha 1.034 1.067 165.3 7.10 6.33 
Li3F41.041 1.041 180.0 6.95 6.95 
LiF4H4 1.035 1.042 175.5 7.33 7.06 
Li2F31.041 1.041 180.0 6.96 6.96 
LiF31.014 1.079 180.0 7.81 6.22 
a

Linear and bent bifluoride anions are present in this phase.

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